P
US7188033B2ExpiredUtilityPatentIndex 92

Method and system of computing and rendering the nature of the chemical bond of hydrogen-type molecules and molecular ions

Assignee: BLACKLIGHT POWER INCPriority: Jul 21, 2003Filed: Jul 19, 2004Granted: Mar 6, 2007
Est. expiryJul 21, 2023(expired)· nominal 20-yr term from priority
Inventors:MILLS RANDELL L
C01B 3/00Y10T436/24G01N 31/00
92
PatentIndex Score
26
Cited by
198
References
53
Claims

Abstract

Provided is a system of computing and rendering a nature of a chemical bond based on physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions. The system includes a processor for processing Maxwellian equations representing charge, mass, and current density functions of hydrogen-type molecules and molecular ions and an output device in communication with the processor for displaying the nature of the chemical bond.

Claims

exact text as granted — not AI-modified
1. A system of computing and rendering a nature of a chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, said system comprising:
 processing means for processing Maxwellian equations representing charge, mass, and current density functions of hydrogen-type molecules and molecular ions, and; 
 an output device in communication with the processing means for displaying the nature of the chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, wherein the physical, Maxwellian solutions of the charge, mass, and current density functions of hydrogen-type molecules and molecular ions comprises a solution of the classical wave equation 
 
     
       
         
           
             
               
                 [ 
                 
                   
                     
                       ∇ 
                       2 
                     
                     ⁢ 
                     
                       - 
                       
                         1 
                         
                           v 
                           2 
                         
                       
                     
                   
                   ⁢ 
                   
                     
                       ∂ 
                       2 
                     
                     
                       ∂ 
                       
                         t 
                         2 
                       
                     
                   
                 
                 ] 
               
               ⁢ 
               
                 ρ 
                 ⁡ 
                 
                   ( 
                   
                     r 
                     , 
                     θ 
                     , 
                     ϕ 
                     , 
                     t 
                   
                   ) 
                 
               
             
             = 
             0. 
           
         
       
     
   
   
     2. A system of computing and rendering a nature of a chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, said system comprising:
 processing means for processing Maxwellan equations representing charge, mass, and current density functions of hydrogen-type molecules and molecular ions, and; 
 an output device in communication with the processing means for displaying the nature of the chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, wherein the hydrogen molecular ion charge and current density functions, bond distance, and energies are solved from the Laplacian in ellipsoidal coordinates: 
 
     
       
         
           
             
               
                 
                   ( 
                   
                     η 
                     - 
                     ζ 
                   
                   ) 
                 
                 ⁢ 
                 
                   R 
                   ξ 
                 
                 ⁢ 
                 
                   ∂ 
                   
                     ∂ 
                     ξ 
                   
                 
                 ⁢ 
                 
                   ( 
                   
                     
                       R 
                       ξ 
                     
                     ⁢ 
                     
                       
                         ∂ 
                         ϕ 
                       
                       
                         ∂ 
                         ξ 
                       
                     
                   
                   ) 
                 
               
               + 
               
                 
                   ( 
                   
                     ζ 
                     - 
                     ξ 
                   
                   ) 
                 
                 ⁢ 
                 
                   R 
                   η 
                 
                 ⁢ 
                 
                   ∂ 
                   
                     ∂ 
                     η 
                   
                 
                 ⁢ 
                 
                   ( 
                   
                     
                       R 
                       η 
                     
                     ⁢ 
                     
                       
                         ∂ 
                         ϕ 
                       
                       
                         ∂ 
                         η 
                       
                     
                   
                   ) 
                 
               
               + 
               
                 
                   ( 
                   
                     ξ 
                     - 
                     η 
                   
                   ) 
                 
                 ⁢ 
                 
                   R 
                   ζ 
                 
                 ⁢ 
                 
                   ∂ 
                   
                     ∂ 
                     ζ 
                   
                 
                 ⁢ 
                 
                   ( 
                   
                     
                       R 
                       ζ 
                     
                     ⁢ 
                     
                       
                         ∂ 
                         ϕ 
                       
                       
                         ∂ 
                         ζ 
                       
                     
                   
                   ) 
                 
               
             
             = 
             0. 
           
         
       
        with the constraint of nonradiation. 
     
   
   
     3. A system of computing and rendering a nature of a chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydroqen-type molecules and molecular ions, said system comprising:
 processing means for processing Maxwellian equations representing charge, mass, and current density functions of hydrogen-type molecules and molecular ions, and; 
 an output device in communication with the processing means for displaying the nature of the chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, wherein the hydrogen molecular charge and current density functions, bond distance, and energies are solved from the Laplacian in ellipsoidal coordinates: 
 
     
       
         
           
             
               
                 
                   ( 
                   
                     η 
                     - 
                     ζ 
                   
                   ) 
                 
                 ⁢ 
                 
                   R 
                   ξ 
                 
                 ⁢ 
                 
                   ∂ 
                   
                     ∂ 
                     ξ 
                   
                 
                 ⁢ 
                 
                   ( 
                   
                     
                       R 
                       ξ 
                     
                     ⁢ 
                     
                       
                         ∂ 
                         ϕ 
                       
                       
                         ∂ 
                         ξ 
                       
                     
                   
                   ) 
                 
               
               + 
               
                 
                   ( 
                   
                     ζ 
                     - 
                     ξ 
                   
                   ) 
                 
                 ⁢ 
                 
                   R 
                   η 
                 
                 ⁢ 
                 
                   ∂ 
                   
                     ∂ 
                     η 
                   
                 
                 ⁢ 
                 
                   ( 
                   
                     
                       R 
                       η 
                     
                     ⁢ 
                     
                       
                         ∂ 
                         ϕ 
                       
                       
                         ∂ 
                         η 
                       
                     
                   
                   ) 
                 
               
               + 
               
                 
                   ( 
                   
                     ξ 
                     - 
                     η 
                   
                   ) 
                 
                 ⁢ 
                 
                   R 
                   ζ 
                 
                 ⁢ 
                 
                   ∂ 
                   
                     ∂ 
                     ζ 
                   
                 
                 ⁢ 
                 
                   ( 
                   
                     
                       R 
                       ζ 
                     
                     ⁢ 
                     
                       
                         ∂ 
                         ϕ 
                       
                       
                         ∂ 
                         ζ 
                       
                     
                   
                   ) 
                 
               
             
             = 
             0 
           
         
       
        with the constraint of nonradiation. 
     
   
   
     4. A system of computing and rendering a nature of a chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, said system comprising:
 processing means for processing Maxwellian equations representing charge, mass, and current density functions of hydrogen-type molecules and molecular ions, and; 
 an output device in communication with the processing means for displaying the nature of the chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, wherein the hydrogen molecular ion charge and current density functions, bond distance, and energies are solved from the Laplacian in ellipsoidal coordinates: 
 
     
       
         
           
             
               
                 
                   ( 
                   
                     η 
                     - 
                     ζ 
                   
                   ) 
                 
                 ⁢ 
                 
                   R 
                   ξ 
                 
                 ⁢ 
                 
                   ∂ 
                   
                     ∂ 
                     ξ 
                   
                 
                 ⁢ 
                 
                   ( 
                   
                     
                       R 
                       ξ 
                     
                     ⁢ 
                     
                       
                         ∂ 
                         ϕ 
                       
                       
                         ∂ 
                         ξ 
                       
                     
                   
                   ) 
                 
               
               + 
               
                 
                   ( 
                   
                     ζ 
                     - 
                     ξ 
                   
                   ) 
                 
                 ⁢ 
                 
                   R 
                   η 
                 
                 ⁢ 
                 
                   ∂ 
                   
                     ∂ 
                     η 
                   
                 
                 ⁢ 
                 
                   ( 
                   
                     
                       R 
                       η 
                     
                     ⁢ 
                     
                       
                         ∂ 
                         ϕ 
                       
                       
                         ∂ 
                         η 
                       
                     
                   
                   ) 
                 
               
               + 
               
                 
                   ( 
                   
                     ξ 
                     - 
                     η 
                   
                   ) 
                 
                 ⁢ 
                 
                   R 
                   ζ 
                 
                 ⁢ 
                 
                   ∂ 
                   
                     ∂ 
                     ζ 
                   
                 
                 ⁢ 
                 
                   ( 
                   
                     
                       R 
                       ζ 
                     
                     ⁢ 
                     
                       
                         ∂ 
                         ϕ 
                       
                       
                         ∂ 
                         ζ 
                       
                     
                   
                   ) 
                 
               
             
             = 
             0 
           
         
       
        with the constraint of nonradiation. 
     
   
   
     5. A system of computing and rendering a nature of a chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, said system comprising:
 processing means for processing Maxwellian equations representing charge, mass, and current density functions of hydrogen-type molecules and molecular ions, and; 
 an output device in communication with the processing means for displaying the nature of the chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, wherein the hydrogen molecular charge and current density functions, bond distance, and energies are solved from the Laplacian in ellipsoidal coordinates: 
 
     
       
         
           
             
               
                 
                   ( 
                   
                     η 
                     - 
                     ζ 
                   
                   ) 
                 
                 ⁢ 
                 
                   R 
                   ξ 
                 
                 ⁢ 
                 
                   ∂ 
                   
                     ∂ 
                     ξ 
                   
                 
                 ⁢ 
                 
                   ( 
                   
                     
                       R 
                       ξ 
                     
                     ⁢ 
                     
                       
                         ∂ 
                         ϕ 
                       
                       
                         ∂ 
                         ξ 
                       
                     
                   
                   ) 
                 
               
               + 
               
                 
                   ( 
                   
                     ζ 
                     - 
                     ξ 
                   
                   ) 
                 
                 ⁢ 
                 
                   R 
                   η 
                 
                 ⁢ 
                 
                   ∂ 
                   
                     ∂ 
                     η 
                   
                 
                 ⁢ 
                 
                   ( 
                   
                     
                       R 
                       η 
                     
                     ⁢ 
                     
                       
                         ∂ 
                         ϕ 
                       
                       
                         ∂ 
                         η 
                       
                     
                   
                   ) 
                 
               
               + 
               
                 
                   ( 
                   
                     ξ 
                     - 
                     η 
                   
                   ) 
                 
                 ⁢ 
                 
                   R 
                   ζ 
                 
                 ⁢ 
                 
                   ∂ 
                   
                     ∂ 
                     ζ 
                   
                 
                 ⁢ 
                 
                   ( 
                   
                     
                       R 
                       ζ 
                     
                     ⁢ 
                     
                       
                         ∂ 
                         ϕ 
                       
                       
                         ∂ 
                         ζ 
                       
                     
                   
                   ) 
                 
               
             
             = 
             0 
           
         
       
        with the constraint of nonradiation. 
     
   
   
     6. A system of computing and rendering a nature of a chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, said system comprising:
 processing means for processing Maxwellian equations representing charge, mass, and current density functions of hydrogen-type molecules and molecular ions, and; 
 an output device in communication with the processing means for displaying the nature of the chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, wherein a vibrational energy of hydrogen molecular ion H 2   + (1/p) having a central field of +pe at each focus of the prolate spheroid molecular orbital is
     E   vib (1)= p   2 0.270 eV; 
 
  and the rotational energy absorbed by a hydrogen-type molecular ion with the transition from the state with the rotational quantum number J to one with the rotational quantum number J+1 is 
 
     
       
         
           
             
               
                 
                   
                     Δ 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     E 
                   
                   = 
                   
                     
                       E 
                       
                         J 
                         + 
                         1 
                       
                     
                     - 
                     
                       E 
                       J 
                     
                   
                 
               
             
             
               
                 
                   = 
                   
                     
                       
                         
                           p 
                           2 
                         
                         ⁢ 
                         
                           ℏ 
                           2 
                         
                       
                       
                         
                           m 
                           p 
                         
                         ⁢ 
                         2 
                         ⁢ 
                         
                           a 
                           H 
                           2 
                         
                       
                     
                     ⁡ 
                     
                       [ 
                       
                         J 
                         + 
                         1 
                       
                       ] 
                     
                   
                 
               
             
             
               
                 
                   = 
                   
                     
                       
                         p 
                         2 
                       
                       ⁡ 
                       
                         [ 
                         
                           J 
                           + 
                           1 
                         
                         ] 
                       
                     
                     ⁢ 
                     1.186 
                     ⁢ 
                     
                         
                     
                     × 
                     
                       10 
                       
                         - 
                         21 
                       
                     
                   
                 
               
             
             
               
                 
                   J 
                   = 
                   
                     
                       
                         p 
                         2 
                       
                       ⁡ 
                       
                         [ 
                         
                           J 
                           + 
                           1 
                         
                         ] 
                       
                     
                     ⁢ 
                     0.00740 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     eV 
                   
                 
               
             
           
         
       
     
   
   
     7. A system of computing and rendering a nature of a chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, said system comprising:
 processing means for processing Maxwellian equations representing charge, mass, and current density functions of hydrogen-type molecules and molecular ions, and; 
 an output device in communication with the processing means for displaying the nature of the chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, wherein a vibrational energy of hydrogen-type molecule H 2 (1/p) having a central field of +pe at each focus of the prolate spheroid molecular orbital is
     E   vib (1)= p   2 0.517 eV; 
 
  and the rotational energy absorbed by a hydrogen-type molecule with the transition from the state with the rotational quantum number J to one with the rotational quantum number J+1 is 
 
     
       
         
           
             
               
                 
                   
                     Δ 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     E 
                   
                   = 
                     
                   ⁢ 
                   
                     
                       
                         E 
                         
                           J 
                           + 
                           1 
                         
                       
                       - 
                       
                         E 
                         J 
                       
                     
                     = 
                     
                       
                         
                           
                             p 
                             2 
                           
                           ⁢ 
                           
                             h 
                             2 
                           
                         
                         
                           
                             m 
                             p 
                           
                           ⁢ 
                           
                             a 
                             o 
                             2 
                           
                         
                       
                       ⁡ 
                       
                         [ 
                         
                           J 
                           + 
                           1 
                         
                         ] 
                       
                     
                   
                 
               
             
             
               
                 
                   = 
                     
                   ⁢ 
                   
                     
                       
                         p 
                         2 
                       
                       ⁡ 
                       
                         [ 
                         
                           J 
                           + 
                           1 
                         
                         ] 
                       
                     
                     ⁢ 
                     2.37 
                     × 
                     
                       10 
                       
                         - 
                         21 
                       
                     
                   
                 
               
             
             
               
                 
                   J 
                   = 
                     
                   ⁢ 
                   
                     
                       
                         p 
                         2 
                       
                       ⁡ 
                       
                         [ 
                         
                           J 
                           + 
                           1 
                         
                         ] 
                       
                     
                     ⁢ 
                     0.0148 
                     ⁢ 
                     eV 
                   
                 
               
             
           
         
       
     
   
   
     8. A system of computing and rendering a nature of a chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, said system comprising:
 processing means for processing Maxwellian equations representing charge, mass, and current density functions of hydrogen-type molecules and molecular ions, and; 
 an output device in communication with the processing means for displaying the nature of the chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, wherein a chemical shift 
 
     
       
         
           
             
               Δ 
               ⁢ 
               
                   
               
               ⁢ 
               B 
             
             B 
           
         
       
        of H 2  relative to a bare proton is given by 
     
     
       
         
           
             
               
                 
                   
                     
                       Δ 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       B 
                     
                     B 
                   
                   = 
                     
                   ⁢ 
                   
                     
                       
                         Δ 
                         ⁢ 
                         
                             
                         
                         ⁢ 
                         B 
                       
                       B 
                     
                     = 
                     
                       
                         - 
                         
                           
                             μ 
                             0 
                           
                           ⁡ 
                           
                             ( 
                             
                               
                                 
                                   
                                     p 
                                     3 
                                   
                                   ⁢ 
                                   4 
                                 
                                 
                                   a 
                                   0 
                                   3 
                                 
                               
                               - 
                               
                                 
                                   
                                     
                                       p 
                                       3 
                                     
                                     ⁢ 
                                     
                                       2 
                                     
                                   
                                   
                                     a 
                                     0 
                                     3 
                                   
                                 
                                 ⁢ 
                                 ln 
                                 ⁢ 
                                 
                                   
                                     
                                       2 
                                     
                                     + 
                                     1 
                                   
                                   
                                     
                                       2 
                                     
                                     - 
                                     1 
                                   
                                 
                               
                             
                             ) 
                           
                         
                       
                       ⁢ 
                       
                         
                           
                             a 
                             0 
                             3 
                           
                           ⁢ 
                           
                             ⅇ 
                             2 
                           
                         
                         
                           36 
                           ⁢ 
                           
                             p 
                             2 
                           
                           ⁢ 
                           
                             m 
                             e 
                           
                         
                       
                     
                   
                 
               
             
             
               
                 
                   = 
                     
                   ⁢ 
                   
                     
                       - 
                       
                         
                           μ 
                           0 
                         
                         ⁡ 
                         
                           ( 
                           
                             4 
                             - 
                             
                               
                                 2 
                               
                               ⁢ 
                               ln 
                               ⁢ 
                               
                                 
                                   
                                     2 
                                   
                                   + 
                                   1 
                                 
                                 
                                   
                                     2 
                                   
                                   - 
                                   1 
                                 
                               
                             
                           
                           ) 
                         
                       
                     
                     ⁢ 
                     
                       
                         pⅇ 
                         2 
                       
                       
                         36 
                         ⁢ 
                         
                           a 
                           0 
                         
                         ⁢ 
                         
                           m 
                           e 
                         
                       
                     
                   
                 
               
             
             
               
                 
                   = 
                     
                   ⁢ 
                   
                     
                       - 
                       p28 
                     
                     ⁢ 
                     .01 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     ppm 
                   
                 
               
             
           
         
       
        where p=1 for H 2 . 
     
   
   
     9. A system of computing and rendering a nature of a chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hydrogen-type molecules and molecular ions, said system comprising:
 processing means for processing Maxwellian equations representing charge, mass, and current density functions of hydrogen-type molecules and molecular ions, and; 
 an output device in communication with the processing means for displaying the nature, of the chemical bond comprising physical, Maxwellian solutions of charge, mass, and current density functions of hvdroaen-type molecules and molecular ions, wherein a total NMR shift 
 
     
       
         
           
             
               
                 Δ 
                 ⁢ 
                 
                     
                 
                 ⁢ 
                 
                   B 
                   T 
                 
               
               B 
             
             , 
           
         
       
        of the hydrogen molecule H 2 (1/p) having a central field of +pe at each focus of the prolate spheroid molecular orbital is given by the sum of that of H 2  plus a relativistic component: 
     
     
       
         
           
             
               
                 
                   
                     
                       Δ 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       
                         B 
                         T 
                       
                     
                     B 
                   
                   = 
                     
                   ⁢ 
                   
                     
                       - 
                       
                         
                           μ 
                           0 
                         
                         ⁡ 
                         
                           ( 
                           
                             4 
                             - 
                             
                               
                                 2 
                               
                               ⁢ 
                               ln 
                               ⁢ 
                               
                                 
                                   
                                     2 
                                   
                                   + 
                                   1 
                                 
                                 
                                   
                                     2 
                                   
                                   - 
                                   1 
                                 
                               
                             
                           
                           ) 
                         
                       
                     
                     ⁢ 
                     
                       
                         ⅇ 
                         2 
                       
                       
                         36 
                         ⁢ 
                         
                           a 
                           0 
                         
                         ⁢ 
                         
                           m 
                           e 
                         
                       
                     
                     ⁢ 
                     
                       ( 
                       
                         1 
                         + 
                         
                           πα 
                           ⁢ 
                           
                               
                           
                           ⁢ 
                           p 
                         
                       
                       ) 
                     
                   
                 
               
             
             
               
                 
                   
                     
                       Δ 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       
                         B 
                         T 
                       
                     
                     B 
                   
                   = 
                     
                   ⁢ 
                   
                     
                       - 
                       
                         ( 
                         
                           28.01 
                           + 
                           
                             0.64 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             p 
                           
                         
                         ) 
                       
                     
                     ⁢ 
                     ppm 
                   
                 
               
             
           
         
       
        where p=integer>1. 
     
   
   
     10. The system of any one of  claims 1 ,  2 ,  3 ,  4 ,  5 , and  6 – 9 , wherein the output device is a display that displays at least one of visual or graphical media. 
   
   
     11. The system of  claim 10  wherein the display is at least one of static or dynamic. 
   
   
     12. The system of  claim 11  wherein at least one of vibration and rotation is be displayed. 
   
   
     13. The system of any one of  claims 1 ,  2 ,  3 ,  4 ,  5 , and  6 – 9 , wherein displayed information is used to model reactivity and physical properties. 
   
   
     14. The system of any one of  claims 1 ,  2 ,  3 ,  4 ,  5 , and  6 – 9 , wherein the output device is a monitor, video projector, printer, or three-dimensional rendering device. 
   
   
     15. The system of any one of  claims 1 ,  2 ,  3 ,  4 ,  5 , and  6 – 9 , wherein displayed information is used to model other molecules and provides utility to anticipate their reactivity and physical properties. 
   
   
     16. The system of any one of  claims 1 ,  2 ,  3 ,  4 ,  5 , and  6 – 9 , wherein the processing means is a general purpose computer. 
   
   
     17. The system of  claim 16  wherein the general purpose computer comprises a central processing unit (CPU), one or more specialized processors, system memory, a mass storage device such as a magnetic disk, an optical disk, or other storage device, an input means. 
   
   
     18. The system of  claim 17 , wherein the input means comprises a serial port, usb port, microphone input, camera input, keyboard or mouse. 
   
   
     19. The system of any one of  claims 1 ,  2 ,  3 ,  4 ,  5 , and  6 – 9 , wherein the processing means comprises a special purpose computer or other hardware system. 
   
   
     20. The system of any one of  claims 1 ,  2 ,  3 ,  4 ,  5 , and  6 – 9 , further comprising computer program products. 
   
   
     21. The system of  claim 20  comprising computer readable medium having embodied therein program code means. 
   
   
     22. The system of  claim 21  wherein the computer readable media is any available media which can be accessed by a general purpose or special purpose computer. 
   
   
     23. The system of  claim 22  wherein the computer readable media comprises at least one of RAM, ROM, EPROM, CD ROM, DVD or other optical disk storage, magnetic disk storage or other magnetic storage devices, or any other medium which can embody the desired program code means and which can be accessed by a general purpose or special purpose computer. 
   
   
     24. The system of  claim 23  wherein the program code means comprises executable instructions and data which cause a general purpose computer or special purpose computer to perform a certain function of a group of functions. 
   
   
     25. The system of  claim 24  wherein the program code is Mathematica programmed with an algorithm based on the physical solutions, and the computer is a PC. 
   
   
     26. The system of  claim 25  wherein the algorithm is ParametricPlot3D[{2*Sqrt[1−z*z]*Cos[u],Sqrt[(1−z*z)]*Sin [u],z}{u,0,2*Pi},{z,−1,9999}], and the rendering is viewed from different perspectives. 
   
   
     27. The system of  claim 26  wherein the algorithms for viewing from different perspectives comprises Show[Out[1], ViewPoint- 22  {x,y,z}] where x, y, and z are Cartesian coordinates. 
   
   
     28. The system of  claim 1  wherein the boundary constraint of the wave equation solution is nonradiation according to Maxwell's equations. 
   
   
     29. The system of  claim 28  wherein a boundary condition is met for an ellipsoidal-time harmonic function when 
     
       
         
           
             
               ω 
               n 
             
             = 
             
               
                 
                   π 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   ℏ 
                 
                 
                   
                     m 
                     e 
                   
                   ⁢ 
                   A 
                 
               
               = 
               
                 ℏ 
                 
                   
                     m 
                     e 
                   
                   ⁢ 
                   ab 
                 
               
             
           
         
       
        where the area of an ellipse is
   A=πab 
 
        where 2b is the length of the semiminor axis and 2a is the length of the semimajor axis. 
     
   
   
     30. The system of  claim 2  wherein a force balance equation for the hydrogen molecular ion is 
     
       
         
           
             
               
                 
                   ℏ 
                   2 
                 
                 
                   
                     m 
                     e 
                   
                   ⁢ 
                   
                     a 
                     2 
                   
                   ⁢ 
                   
                     b 
                     2 
                   
                 
               
               ⁢ 
               2 
               ⁢ 
               
                 ab 
                 2 
               
               ⁢ 
               X 
             
             = 
             
               
                 
                   e 
                   2 
                 
                 
                   4 
                   ⁢ 
                   
                     πɛ 
                     o 
                   
                 
               
               ⁢ 
               X 
             
           
         
       
     
     where 
     
       
         
           
             X 
             = 
             
               
                 1 
                 
                   
                     ξ 
                     + 
                     
                       a 
                       2 
                     
                   
                 
               
               ⁢ 
               
                 1 
                 
                   
                     ξ 
                     + 
                     
                       b 
                       2 
                     
                   
                 
               
               ⁢ 
               
                 1 
                 c 
               
               ⁢ 
               
                 
                   
                     
                       
                         ξ 
                         2 
                       
                       - 
                       1 
                     
                     
                       
                         ξ 
                         2 
                       
                       - 
                       
                         η 
                         2 
                       
                     
                   
                 
                 . 
               
             
           
         
       
     
   
   
     31. The system of  claim 30  wherein the force balance equation has the parametric solution
     r ( t )= a  cos ω t+jb  sin ω t   
 
     when the semimajor axis, a, is
   a=2a o . 
 
   
   
     32. The system of  claim 31  wherein an internuclear distance, 2c′, which is the distance between the foci is
   2c′=2a o ; 
 
     the semiminor axis is
     b √{square root over (3)} a   o , and 
 
     the eccentricity, e, is 
     
       
         
           
             e 
             = 
             
               
                 1 
                 2 
               
               . 
             
           
         
       
     
   
   
     33. The system of  claim 32  wherein a potential energy of the electron in the central field of the protons at the foci is 
     
       
         
           
             
               
                 V 
                 e 
               
               = 
               
                 
                   
                     
                       
                         - 
                         4 
                       
                       ⁢ 
                       
                         e 
                         2 
                       
                     
                     
                       8 
                       ⁢ 
                       π 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       
                         ɛ 
                         0 
                       
                       ⁢ 
                       
                         
                           
                             a 
                             2 
                           
                           - 
                           
                             b 
                             2 
                           
                         
                       
                     
                   
                   ⁢ 
                   ln 
                   ⁢ 
                   
                     
                       a 
                       + 
                       
                         
                           
                             a 
                             2 
                           
                           - 
                           
                             b 
                             2 
                           
                         
                       
                     
                     
                       a 
                       - 
                       
                         
                           
                             a 
                             2 
                           
                           - 
                           
                             b 
                             2 
                           
                         
                       
                     
                   
                 
                 = 
                 
                   
                     - 
                     59.7575 
                   
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   eV 
                 
               
             
             ; 
           
         
       
     
     The potential energy of the two protons is 
     
       
         
           
             
               
                 V 
                 p 
               
               = 
               
                 
                   
                     e 
                     2 
                   
                   
                     8 
                     ⁢ 
                     π 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     
                       ɛ 
                       0 
                     
                     ⁢ 
                     
                       a 
                       H 
                     
                   
                 
                 = 
                 
                   13.5984 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   eV 
                 
               
             
             , 
             and 
           
         
       
     
     The kinetic energy of the electron is 
     
       
         
           
             T 
             = 
             
               
                 
                   
                     2 
                     ⁢ 
                     
                       ℏ 
                       2 
                     
                   
                   
                     
                       m 
                       e 
                     
                     ⁢ 
                     a 
                     ⁢ 
                     
                       
                         
                           a 
                           2 
                         
                         - 
                         
                           b 
                           2 
                         
                       
                     
                   
                 
                 ⁢ 
                 ln 
                 ⁢ 
                 
                   
                     
                         
                     
                     ⁢ 
                     
                       a 
                       + 
                       
                         
                           
                             a 
                             2 
                           
                           - 
                           
                             b 
                             2 
                           
                         
                       
                     
                   
                   
                     a 
                     - 
                     
                       
                         
                           a 
                           2 
                         
                         - 
                         
                           b 
                           2 
                         
                       
                     
                   
                 
               
               = 
               
                 29.8787 
                 ⁢ 
                 
                     
                 
                 ⁢ 
                 
                   eV 
                   . 
                 
               
             
           
         
       
     
   
   
     34. The system of  claim 33  wherein during bond formation, the electron undergoes a reentrant oscillatory orbit with vibration of the protons, and the corresponding energy Ē osc  is the difference between the Doppler and average vibrational kinetic energies: 
     
       
         
           
             
               
                 
                   E 
                   _ 
                 
                 osc 
               
               = 
               
                 
                   
                     
                       E 
                       _ 
                     
                     D 
                   
                   + 
                   
                     
                       E 
                       _ 
                     
                     Kvib 
                   
                 
                 = 
                 
                   
                     
                       ( 
                       
                         
                           V 
                           o 
                         
                         + 
                         T 
                         + 
                         
                           V 
                           p 
                         
                       
                       ) 
                     
                     ⁢ 
                     
                       
                         
                           2 
                           ⁢ 
                           
                             
                               E 
                               _ 
                             
                             K 
                           
                         
                         
                           Mc 
                           2 
                         
                       
                     
                   
                   + 
                   
                     
                       1 
                       2 
                     
                     ⁢ 
                     h 
                     ⁢ 
                     
                       
                         k 
                         μ 
                       
                     
                   
                 
               
             
             , 
             
                 
             
             ⁢ 
             and 
           
         
       
     
     The total energy is 
     
       
         
           
             
               
                 
                   
                     E 
                     T 
                   
                   = 
                     
                   ⁢ 
                   
                     
                       V 
                       e 
                     
                     + 
                     T 
                     + 
                     
                       V 
                       p 
                     
                     + 
                     
                       
                         E 
                         _ 
                       
                       osc 
                     
                   
                 
               
             
             
               
                 
                   
                     E 
                     T 
                   
                   = 
                     
                   ⁢ 
                   
                     - 
                     
                       { 
                       
                         
                           
                             
                               
                                 
                                   e 
                                   2 
                                 
                                 
                                   8 
                                   ⁢ 
                                   π 
                                   ⁢ 
                                   
                                       
                                   
                                   ⁢ 
                                   
                                     e 
                                     o 
                                   
                                   ⁢ 
                                   
                                     a 
                                     H 
                                   
                                 
                               
                               ⁢ 
                               
                                 ( 
                                 
                                   
                                     4 
                                     ⁢ 
                                     
                                         
                                     
                                     ⁢ 
                                     ln 
                                     ⁢ 
                                     
                                         
                                     
                                     ⁢ 
                                     3 
                                   
                                   - 
                                   1 
                                   - 
                                   
                                     2 
                                     ⁢ 
                                     
                                         
                                     
                                     ⁢ 
                                     ln 
                                     ⁢ 
                                     
                                         
                                     
                                     ⁢ 
                                     3 
                                   
                                 
                                 ) 
                               
                             
                           
                         
                         
                           
                             
                               
                                 [ 
                                 
                                   1 
                                   + 
                                   
                                     
                                       
                                         2 
                                         ⁢ 
                                         ℏ 
                                         ⁢ 
                                         
                                           
                                             
                                               
                                                 2 
                                                 ⁢ 
                                                 
                                                   e 
                                                   2 
                                                 
                                               
                                               
                                                 4 
                                                 ⁢ 
                                                 
                                                   
                                                     
                                                       pe 
                                                       o 
                                                     
                                                     ⁡ 
                                                     
                                                       ( 
                                                       
                                                         2 
                                                         ⁢ 
                                                         
                                                           a 
                                                           H 
                                                         
                                                       
                                                       ) 
                                                     
                                                   
                                                   3 
                                                 
                                               
                                             
                                             
                                               m 
                                               e 
                                             
                                           
                                         
                                       
                                       
                                         
                                           m 
                                           e 
                                         
                                         ⁢ 
                                         
                                           c 
                                           2 
                                         
                                       
                                     
                                   
                                 
                                 ] 
                               
                               - 
                               
                                 
                                   1 
                                   2 
                                 
                                 ⁢ 
                                 ℏ 
                                 ⁢ 
                                 
                                   
                                     k 
                                     m 
                                   
                                 
                               
                             
                           
                         
                       
                       } 
                     
                   
                 
               
             
             
               
                 
                   = 
                     
                   ⁢ 
                   
                     
                       
                         - 
                         16.2803 
                       
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       eV 
                     
                     - 
                     
                       0.118811 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       eV 
                     
                     + 
                     
                       
                         1 
                         2 
                       
                       ⁢ 
                       
                         ( 
                         
                           0.29282 
                           ⁢ 
                           
                               
                           
                           ⁢ 
                           eV 
                         
                         ) 
                       
                     
                   
                 
               
             
             
               
                 
                   = 
                     
                   ⁢ 
                   
                     
                       - 
                       16.2527 
                     
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     eV 
                   
                 
               
             
           
         
       
     
   
   
     35. The system of  claim 34  wherein a bond dissociation energy, E D , is the difference between the total energy of the hydrogen atom and E T :
     E   D   =E ( H )− E   T =2.654 eV 
 
     wherein the total energy of a hydrogen atom is
     E ( H )=−13.59844 eV. 
 
   
   
     36. The system of  claim 3  wherein a force balance equation for the hydrogen molecule is 
     
       
         
           
             
               
                 
                   ℏ 
                   2 
                 
                 
                   
                     m 
                     e 
                   
                   ⁢ 
                   
                     a 
                     2 
                   
                   ⁢ 
                   
                     b 
                     2 
                   
                 
               
               ⁢ 
               2 
               ⁢ 
               
                 ab 
                 2 
               
               ⁢ 
               X 
             
             = 
             
               
                 
                   
                     e 
                     2 
                   
                   
                     4 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     π 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     
                       ɛ 
                       o 
                     
                   
                 
                 ⁢ 
                 X 
               
               + 
               
                 
                   
                     ℏ 
                     2 
                   
                   
                     2 
                     ⁢ 
                     
                       m 
                       e 
                     
                     ⁢ 
                     
                       a 
                       2 
                     
                     ⁢ 
                     
                       b 
                       2 
                     
                   
                 
                 ⁢ 
                 2 
                 ⁢ 
                 
                   ab 
                   2 
                 
                 ⁢ 
                 X 
               
             
           
         
       
     
     where 
     
       
         
           
             X 
             = 
             
               
                 1 
                 
                   
                     ξ 
                     + 
                     
                       a 
                       2 
                     
                   
                 
               
               ⁢ 
               
                 1 
                 
                   
                     ξ 
                     + 
                     
                       b 
                       2 
                     
                   
                 
               
               ⁢ 
               
                 1 
                 c 
               
               ⁢ 
               
                 
                   
                     
                       
                         ξ 
                         2 
                       
                       - 
                       1 
                     
                     
                       
                         ξ 
                         2 
                       
                       - 
                       
                         η 
                         2 
                       
                     
                   
                 
                 . 
               
             
           
         
       
     
   
   
     37. The system of  claim 36  wherein the force balance equation has the parametric solution
     r ( t )= ia  cos ω t+jb  sin ω t   
 
     when the semimajor axis, a, is
   a=a o . 
 
   
   
     38. The system of  claim 37  wherein an internuclear distance, 2c′, which is the distance between the foci is
   2 c′= √{square root over (2)} a   o ; 
 
     the semiminor axis is 
     
       
         
           
             
               b 
               = 
               
                 
                   1 
                   
                     2 
                   
                 
                 ⁢ 
                 
                   a 
                   o 
                 
               
             
             , 
             and 
           
         
       
     
     the eccentricity, e, is 
     
       
         
           
             e 
             = 
             
               
                 1 
                 
                   2 
                 
               
               . 
             
           
         
       
     
   
   
     39. The system of  claim 38  wherein a potential energy of the two electrons in the central field of the protons at the foci is 
     
       
         
           
             
               
                 V 
                 e 
               
               = 
               
                 
                   
                     
                       
                         - 
                         2 
                       
                       ⁢ 
                       
                         e 
                         2 
                       
                     
                     
                       8 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       π 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       
                         ɛ 
                         o 
                       
                       ⁢ 
                       
                         
                           
                             a 
                             2 
                           
                           - 
                           
                             b 
                             2 
                           
                         
                       
                     
                   
                   ⁢ 
                   ln 
                   ⁢ 
                   
                     
                       a 
                       + 
                       
                         
                           
                             a 
                             2 
                           
                           - 
                           
                             b 
                             2 
                           
                         
                       
                     
                     
                       a 
                       - 
                       
                         
                           
                             a 
                             2 
                           
                           - 
                           
                             b 
                             2 
                           
                         
                       
                     
                   
                 
                 = 
                 
                   
                     - 
                     67.836 
                   
                   ⁢ 
                   e 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   V 
                 
               
             
             ; 
           
         
       
     
     The potential energy of the two protons is 
     
       
         
           
             
               
                 V 
                 p 
               
               = 
               
                 
                   
                     e 
                     2 
                   
                   
                     8 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     π 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     
                       ɛ 
                       o 
                     
                     ⁢ 
                     
                       
                         
                           a 
                           2 
                         
                         - 
                         
                           b 
                           2 
                         
                       
                     
                   
                 
                 = 
                 
                   19.242 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   e 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   V 
                 
               
             
             ; 
           
         
       
     
     The kinetic energy of the electrons is 
     
       
         
           
             
               T 
               = 
               
                 
                   
                     
                       ℏ 
                       2 
                     
                     
                       2 
                       ⁢ 
                       
                         m 
                         e 
                       
                       ⁢ 
                       a 
                       ⁢ 
                       
                         
                           
                             a 
                             2 
                           
                           - 
                           
                             b 
                             2 
                           
                         
                       
                     
                   
                   ⁢ 
                   ln 
                   ⁢ 
                   
                     
                       a 
                       + 
                       
                         
                           
                             a 
                             2 
                           
                           - 
                           
                             b 
                             2 
                           
                         
                       
                     
                     
                       a 
                       - 
                       
                         
                           
                             a 
                             2 
                           
                           - 
                           
                             b 
                             2 
                           
                         
                       
                     
                   
                 
                 = 
                 
                   33.918 
                   ⁢ 
                   e 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   V 
                 
               
             
             , 
             
                 
             
             ⁢ 
             and 
           
         
       
     
     The energy, V m , of the magnetic force between the electrons is 
     
       
         
           
             
               V 
               m 
             
             = 
             
               
                 
                   
                     ℏ 
                     2 
                   
                   
                     4 
                     ⁢ 
                     
                       m 
                       e 
                     
                     ⁢ 
                     a 
                     ⁢ 
                     
                       
                         
                           a 
                           2 
                         
                         - 
                         
                           b 
                           2 
                         
                       
                     
                   
                 
                 ⁢ 
                 ln 
                 ⁢ 
                 
                   
                     a 
                     + 
                     
                       
                         
                           a 
                           2 
                         
                         - 
                         
                           b 
                           2 
                         
                       
                     
                   
                   
                     a 
                     - 
                     
                       
                         
                           a 
                           2 
                         
                         - 
                         
                           b 
                           2 
                         
                       
                     
                   
                 
               
               = 
               
                 
                   - 
                   16.959 
                 
                 ⁢ 
                 e 
                 ⁢ 
                 
                     
                 
                 ⁢ 
                 
                   V 
                   . 
                 
               
             
           
         
       
     
   
   
     40. The system of  claim 39  wherein during bond formation, the electrons undergo a reentrant oscillatory orbit with vibration of the protons, and the corresponding energy Ē osc  is the difference between the Doppler and average vibrational kinetic energies: 
     
       
         
           
             
               
                 
                   E 
                   _ 
                 
                 osc 
               
               = 
               
                 
                   
                     
                       E 
                       _ 
                     
                     D 
                   
                   + 
                   
                     
                       E 
                       _ 
                     
                     Kvib 
                   
                 
                 = 
                 
                   
                     
                       ( 
                       
                         
                           V 
                           e 
                         
                         + 
                         T 
                         + 
                         
                           V 
                           m 
                         
                         + 
                         
                           V 
                           p 
                         
                       
                       ) 
                     
                     ⁢ 
                     
                       
                         
                           2 
                           ⁢ 
                           
                             
                               E 
                               _ 
                             
                             K 
                           
                         
                         
                           Mc 
                           2 
                         
                       
                     
                   
                   + 
                   
                     
                       1 
                       2 
                     
                     ⁢ 
                     ℏ 
                     ⁢ 
                     
                       
                         k 
                         μ 
                       
                     
                   
                 
               
             
             , 
             and 
           
         
       
     
     The total energy is 
     
       
         
           
             
               
                 
                   
                     E 
                     T 
                   
                   = 
                     
                   ⁢ 
                   
                     
                       V 
                       e 
                     
                     + 
                     T 
                     + 
                     
                       V 
                       m 
                     
                     + 
                     
                       V 
                       p 
                     
                     + 
                     
                       
                         E 
                         _ 
                       
                       osc 
                     
                   
                 
               
             
             
               
                 
                   
                     E 
                     T 
                   
                   = 
                     
                   ⁢ 
                   
                     - 
                     
                       
                         
                           e 
                           2 
                         
                         
                           8 
                           ⁢ 
                           
                             πɛ 
                             o 
                           
                           ⁢ 
                           
                             a 
                             0 
                           
                         
                       
                       ⁡ 
                       
                         [ 
                         
                           
                             
                               ( 
                               
                                 
                                   2 
                                   ⁢ 
                                   
                                     2 
                                   
                                 
                                 - 
                                 
                                   2 
                                 
                                 + 
                                 
                                   
                                     2 
                                   
                                   2 
                                 
                               
                               ) 
                             
                             ⁢ 
                             ln 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             
                               
                                 
                                   2 
                                 
                                 + 
                                 1 
                               
                               
                                 
                                   2 
                                 
                                 - 
                                 1 
                               
                             
                           
                           - 
                           
                             2 
                           
                         
                         ] 
                       
                     
                   
                 
               
             
             
               
                 
                     
                   ⁢ 
                   
                     
                       [ 
                       
                         1 
                         + 
                         
                           
                             
                               2 
                               ⁢ 
                               ℏ 
                               ⁢ 
                               
                                 
                                   
                                     
                                       e 
                                       2 
                                     
                                     
                                       4 
                                       ⁢ 
                                       
                                         πɛ 
                                         o 
                                       
                                       ⁢ 
                                       
                                         a 
                                         0 
                                         3 
                                       
                                     
                                   
                                   
                                     m 
                                     e 
                                   
                                 
                               
                             
                             
                               
                                 m 
                                 e 
                               
                               ⁢ 
                               
                                 c 
                                 2 
                               
                             
                           
                         
                       
                       ] 
                     
                     . 
                   
                 
               
             
             
               
                 
                     
                   ⁢ 
                   
                     
                       - 
                       
                         1 
                         2 
                       
                     
                     ⁢ 
                     ℏ 
                     ⁢ 
                     
                       
                         k 
                         μ 
                       
                     
                   
                 
               
             
             
               
                 
                   = 
                     
                   ⁢ 
                   
                     
                       - 
                       31.689 
                     
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     eV 
                   
                 
               
             
           
         
       
     
   
   
     41. The system of  claim 40  wherein a bond dissociation energy, E D , is the difference between the total energy of the hydrogen atoms and E T :
     E   D   =E (2 H[a   H ])− E   T =4.478 eV 
 
     wherein the total energy of two hydrogen atoms is
     E (2 H[a   H ])=−1.27.21 eV. 
 
   
   
     42. The system of  claim 4  wherein a force balance equation the hydrogen molecular ion H 2   + (1/p) having a central field of +pe at each focus of the prolate spheroid molecular orbital is 
     
       
         
           
             
               
                 
                   ℏ 
                   2 
                 
                 
                   
                     m 
                     e 
                   
                   ⁢ 
                   
                     a 
                     2 
                   
                   ⁢ 
                   
                     b 
                     2 
                   
                 
               
               ⁢ 
               2 
               ⁢ 
               
                 ab 
                 2 
               
               ⁢ 
               X 
             
             = 
             
               
                 
                   p 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     e 
                     2 
                   
                 
                 
                   4 
                   ⁢ 
                   
                     πɛ 
                     o 
                   
                 
               
               ⁢ 
               X 
             
           
         
       
     
     where 
     
       
         
           
             X 
             = 
             
               
                 1 
                 
                   
                     ξ 
                     + 
                     
                       a 
                       2 
                     
                   
                 
               
               ⁢ 
               
                 1 
                 
                   
                     ξ 
                     + 
                     
                       b 
                       2 
                     
                   
                 
               
               ⁢ 
               
                 1 
                 c 
               
               ⁢ 
               
                 
                   
                     
                       
                         ξ 
                         2 
                       
                       - 
                       1 
                     
                     
                       
                         ξ 
                         2 
                       
                       - 
                       
                         η 
                         2 
                       
                     
                   
                 
                 . 
               
             
           
         
       
     
   
   
     43. The system of  claim 42  wherein a force balance equation has the parametric solution
     r ( t )= ia  cos ω t+jb  sin ω t   
 
     when the semimajor axis, a, is 
     
       
         
           
             a 
             = 
             
               
                 
                   2 
                   ⁢ 
                   
                     a 
                     0 
                   
                 
                 p 
               
               . 
             
           
         
       
     
   
   
     44. The system of  claim 43  wherein an internuclear distance, 2c′, which is the distance between the foci is 
     
       
         
           
             
               
                 2 
                 ⁢ 
                 
                   c 
                   ′ 
                 
               
               = 
               
                 
                   2 
                   ⁢ 
                   
                     a 
                     o 
                   
                 
                 p 
               
             
             ; 
           
         
       
     
     the semiminor axis is 
     
       
         
           
             
               b 
               = 
               
                 
                   
                     3 
                   
                   p 
                 
                 ⁢ 
                 
                   a 
                   o 
                 
               
             
             , 
             
                 
             
             ⁢ 
             and 
           
         
       
     
     the eccentricity, e, is 
     
       
         
           
             e 
             = 
             
               
                 1 
                 2 
               
               . 
             
           
         
       
     
   
   
     45. The system of  claim 44  wherein a potential energy of the electron in the central field of +pe at the foci is 
     
       
         
           
             
               
                 V 
                 e 
               
               = 
               
                 
                   
                     
                       - 
                       4 
                     
                     ⁢ 
                     
                       p 
                       2 
                     
                     ⁢ 
                     
                       e 
                       2 
                     
                   
                   
                     8 
                     ⁢ 
                     
                       πɛ 
                       o 
                     
                     ⁢ 
                     
                       a 
                       o 
                     
                   
                 
                 ⁢ 
                 ln 
                 ⁢ 
                 
                     
                 
                 ⁢ 
                 3 
               
             
             ; 
           
         
       
     
     The potential energy of the two protons is 
     
       
         
           
             
               
                 V 
                 p 
               
               = 
               
                 
                   
                     p 
                     2 
                   
                   ⁢ 
                   
                     e 
                     2 
                   
                 
                 
                   8 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   π 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     ɛ 
                     o 
                   
                   ⁢ 
                   
                     a 
                     o 
                   
                 
               
             
             , 
             
                 
             
             ⁢ 
             and 
           
         
       
     
     The kinetic energy of the electron is 
     
       
         
           
             T 
             = 
             
               
                 
                   2 
                   ⁢ 
                   
                     p 
                     2 
                   
                   ⁢ 
                   
                     e 
                     2 
                   
                 
                 
                   8 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   π 
                   ⁢ 
                   
                       
                   
                   ⁢ 
                   
                     ɛ 
                     o 
                   
                   ⁢ 
                   
                     a 
                     o 
                   
                 
               
               ⁢ 
               ln 
               ⁢ 
               
                   
               
               ⁢ 
               3. 
             
           
         
       
     
   
   
     46. The system of  claim 45  wherein during bond formation, the electron undergoes a reentrant oscillatory orbit with vibration of the protons, and the corresponding energy Ē osc  is the difference between the Doppler and average vibrational kinetic energies: 
     
       
         
           
             
               
                 
                   E 
                   _ 
                 
                 osc 
               
               = 
               
                 
                   
                     
                       E 
                       _ 
                     
                     D 
                   
                   + 
                   
                     
                       E 
                       _ 
                     
                     Kvib 
                   
                 
                 = 
                 
                   
                     
                       ( 
                       
                         
                           V 
                           c 
                         
                         + 
                         T 
                         + 
                         
                           V 
                           P 
                         
                       
                       ) 
                     
                     ⁢ 
                     
                       
                         
                           2 
                           ⁢ 
                           
                             
                               E 
                               _ 
                             
                             K 
                           
                         
                         
                           Mc 
                           2 
                         
                       
                     
                   
                   + 
                   
                     
                       1 
                       2 
                     
                     ⁢ 
                     h 
                     ⁢ 
                     
                       
                         k 
                         μ 
                       
                     
                   
                 
               
             
             , 
             and 
           
         
       
     
     The total energy of the hydrogen molecular ion H 2   + (1/p) having a central field of +pe at each focus of the prolate spheroid molecular orbital is 
     
       
         
           
             
               
                 
                   
                     E 
                     T 
                   
                   = 
                     
                   ⁢ 
                   
                     
                       V 
                       e 
                     
                     + 
                     T 
                     + 
                     
                       V 
                       P 
                     
                     + 
                     
                       
                         E 
                         _ 
                       
                       osc 
                     
                   
                 
               
             
             
               
                 
                   
                     E 
                     T 
                   
                   = 
                     
                   ⁢ 
                   
                     
                       - 
                       
                         p 
                         2 
                       
                     
                     ⁢ 
                     
                       { 
                       
                         
                           
                             e 
                             2 
                           
                           
                             8 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             π 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             
                               ɛ 
                               o 
                             
                             ⁢ 
                             
                               a 
                               H 
                             
                           
                         
                         ⁢ 
                         
                           ( 
                           
                             
                               4 
                               ⁢ 
                               ln 
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               3 
                             
                             - 
                             1 
                             - 
                             
                               2 
                               ⁢ 
                               ln 
                               ⁢ 
                               
                                   
                               
                               ⁢ 
                               3 
                             
                           
                           ) 
                         
                       
                     
                   
                 
               
             
             
               
                 
                   
                       
                     ⁢ 
                     
                       
                         [ 
                         
                           1 
                           + 
                           
                             p 
                             ⁢ 
                             
                               
                                 
                                   2 
                                   ⁢ 
                                   h 
                                   ⁢ 
                                   
                                     
                                       
                                         
                                           2 
                                           ⁢ 
                                           
                                             e 
                                             2 
                                           
                                         
                                         
                                           
                                             4 
                                             ⁢ 
                                             
                                                 
                                             
                                             ⁢ 
                                             π 
                                             ⁢ 
                                             
                                                 
                                             
                                             ⁢ 
                                             
                                               
                                                 
                                                   ɛ 
                                                   o 
                                                 
                                                 ⁡ 
                                                 
                                                   ( 
                                                   
                                                     2 
                                                     ⁢ 
                                                     
                                                       a 
                                                       H 
                                                     
                                                   
                                                   ) 
                                                 
                                               
                                               3 
                                             
                                           
                                           ⁢ 
                                           
                                               
                                           
                                         
                                       
                                       
                                         m 
                                         e 
                                       
                                     
                                   
                                 
                                 
                                   
                                     m 
                                     c 
                                   
                                   ⁢ 
                                   
                                     c 
                                     2 
                                   
                                 
                               
                             
                           
                         
                         ] 
                       
                       - 
                       
                         
                           1 
                           2 
                         
                         ⁢ 
                         h 
                         ⁢ 
                         
                           
                             k 
                             μ 
                           
                         
                       
                     
                     } 
                   
                   . 
                 
               
             
             
               
                 
                   = 
                     
                   ⁢ 
                   
                     
                       
                         - 
                         
                           p 
                           2 
                         
                       
                       ⁢ 
                       16.13392 
                       ⁢ 
                       eV 
                     
                     - 
                     
                       
                         p 
                         3 
                       
                       ⁢ 
                       0.118755 
                       ⁢ 
                       eV 
                     
                   
                 
               
             
           
         
       
     
   
   
     47. The system of  claim 46  wherein a bond dissociation energy, E D , is the difference between the total energy of the hydrogen atom H(1/p) and E T : 
     
       
         
           
             
               
                 
                   
                     E 
                     D 
                   
                   = 
                   
                     
                       
                         - 
                         
                           p 
                           2 
                         
                       
                       ⁢ 
                       13.59844 
                     
                     - 
                     
                       E 
                       T 
                     
                   
                 
               
             
             
               
                 
                   = 
                   
                     
                       
                         - 
                         
                           p 
                           2 
                         
                       
                       ⁢ 
                       13.59844 
                     
                     - 
                     
                       ( 
                       
                         
                           
                             - 
                             
                               p 
                               2 
                             
                           
                           ⁢ 
                           16.13392 
                           ⁢ 
                           
                               
                           
                           ⁢ 
                           eV 
                         
                         - 
                         
                           
                             p 
                             3 
                           
                           ⁢ 
                           0.118755 
                           ⁢ 
                           
                               
                           
                           ⁢ 
                           eV 
                         
                       
                       ) 
                     
                   
                 
               
             
             
               
                 
                   = 
                   
                     
                       
                         p 
                         2 
                       
                       ⁢ 
                       2.535 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       eV 
                     
                     + 
                     
                       
                         p 
                         3 
                       
                       ⁢ 
                       0.118755 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       eV 
                     
                   
                 
               
             
           
         
       
     
     wherein the total energy of a hydrogen atom H(1/p) is
     E ( H (1 /p ))=− p   2 13.59844 eV. 
 
   
   
     48. The system of  claim 5  wherein a force balance equation for the hydrogen molecule H 2 (1/p) having a central field of +pe at each focus of the prolate spheroid molecular orbital is 
     
       
         
           
             
               
                 
                   h 
                   2 
                 
                 
                   
                     m 
                     e 
                   
                   ⁢ 
                   
                     a 
                     2 
                   
                   ⁢ 
                   
                     b 
                     2 
                   
                 
               
               ⁢ 
               2 
               ⁢ 
               
                 ab 
                 2 
               
               ⁢ 
               X 
             
             = 
             
               
                 
                   
                     p 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     
                       e 
                       2 
                     
                   
                   
                     4 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     π 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     
                       ɛ 
                       o 
                     
                   
                 
                 ⁢ 
                 X 
               
               + 
               
                 
                   
                     h 
                     2 
                   
                   
                     2 
                     ⁢ 
                     
                       m 
                       e 
                     
                     ⁢ 
                     
                       a 
                       2 
                     
                     ⁢ 
                     
                       b 
                       2 
                     
                   
                 
                 ⁢ 
                 2 
                 ⁢ 
                 
                   ab 
                   2 
                 
                 ⁢ 
                 X 
               
             
           
         
       
     
     where 
     
       
         
           
             X 
             = 
             
               
                 1 
                 
                   
                     ξ 
                     + 
                     
                       a 
                       2 
                     
                   
                 
               
               ⁢ 
               
                 1 
                 
                   
                     ξ 
                     + 
                     
                       b 
                       2 
                     
                   
                 
               
               ⁢ 
               
                 1 
                 c 
               
               ⁢ 
               
                 
                   
                     
                       
                         ξ 
                         2 
                       
                       - 
                       1 
                     
                     
                       
                         ξ 
                         2 
                       
                       - 
                       
                         η 
                         2 
                       
                     
                   
                 
                 . 
               
             
           
         
       
     
   
   
     49. The system of  claim 48  wherein the force balance equation has the parametric solution
     r ( t )= ia  cos ω t+jb  sin ω t   
 
     when the semimajor axis, a, is 
     
       
         
           
             a 
             = 
             
               
                 
                   a 
                   o 
                 
                 p 
               
               . 
             
           
         
       
     
   
   
     50. The system of  claim 49  wherein an internuclear distance, 2c′, which is the distance between the foci is 
     
       
         
           
             
               
                 2 
                 ⁢ 
                 
                   c 
                   ′ 
                 
               
               = 
               
                 
                   
                     2 
                   
                   p 
                 
                 ⁢ 
                 
                   a 
                   o 
                 
               
             
             ; 
           
         
       
     
     the semiminor axis is 
     
       
         
           
             
               b 
               = 
               
                 
                   c 
                   ′ 
                 
                 = 
                 
                   
                     1 
                     
                       p 
                       ⁢ 
                       
                         2 
                       
                     
                   
                   ⁢ 
                   
                     a 
                     o 
                   
                 
               
             
             , 
             and 
           
         
       
     
     the eccentricity, e, is 
     
       
         
           
             e 
             = 
             
               
                 1 
                 
                   2 
                 
               
               . 
             
           
         
       
     
   
   
     51. The system of  claim 50  wherein a potential energy of the two electrons in the central field of +pe at the foci is 
     
       
         
           
             
               
                 V 
                 e 
               
               = 
               
                 
                   
                     
                       - 
                       2 
                     
                     ⁢ 
                     p 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     
                       e 
                       2 
                     
                   
                   
                     8 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     π 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     
                       ɛ 
                       o 
                     
                     ⁢ 
                     
                       
                         
                           a 
                           2 
                         
                         - 
                         
                           b 
                           2 
                         
                       
                     
                   
                 
                 ⁢ 
                 ln 
                 ⁢ 
                 
                   
                     a 
                     + 
                     
                       
                         
                           a 
                           2 
                         
                         - 
                         
                           b 
                           2 
                         
                       
                     
                   
                   
                     a 
                     - 
                     
                       
                         
                           a 
                           2 
                         
                         - 
                         
                           b 
                           2 
                         
                       
                     
                   
                 
               
             
             ; 
           
         
       
     
     The potential energy of the two protons is 
     
       
         
           
             
               
                 V 
                 p 
               
               = 
               
                 
                   p 
                   
                     8 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     π 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     
                       ɛ 
                       o 
                     
                   
                 
                 ⁢ 
                 
                   
                     e 
                     2 
                   
                   
                     
                       
                         a 
                         2 
                       
                       - 
                       
                         b 
                         2 
                       
                     
                   
                 
               
             
             ; 
           
         
       
     
     The kinetic energy of the electrons is 
     
       
         
           
             
               T 
               = 
               
                 
                   
                     h 
                     2 
                   
                   
                     2 
                     ⁢ 
                     
                       m 
                       e 
                     
                     ⁢ 
                     a 
                     ⁢ 
                     
                       
                         
                           a 
                           2 
                         
                         - 
                         
                           b 
                           2 
                         
                       
                     
                   
                 
                 ⁢ 
                 ln 
                 ⁢ 
                 
                   
                     a 
                     + 
                     
                       
                         
                           a 
                           2 
                         
                         - 
                         
                           b 
                           2 
                         
                       
                     
                   
                   
                     a 
                     - 
                     
                       
                         
                           a 
                           2 
                         
                         - 
                         
                           b 
                           2 
                         
                       
                     
                   
                 
               
             
             , 
             and 
           
         
       
     
     The energy, V m , of the magnetic force between the electrons is 
     
       
         
           
             
               V 
               m 
             
             = 
             
               
                 
                   - 
                   
                     ℏ 
                     2 
                   
                 
                 
                   4 
                   ⁢ 
                   
                     m 
                     e 
                   
                   ⁢ 
                   a 
                   ⁢ 
                   
                     
                       
                         a 
                         2 
                       
                       - 
                       
                         b 
                         2 
                       
                     
                   
                 
               
               ⁢ 
               ln 
               ⁢ 
               
                 
                   
                     
                         
                     
                     ⁢ 
                     
                       a 
                       + 
                       
                         
                           
                             a 
                             2 
                           
                           - 
                           
                             b 
                             2 
                           
                         
                       
                     
                   
                   
                     a 
                     - 
                     
                       
                         
                           a 
                           2 
                         
                         - 
                         
                           b 
                           2 
                         
                       
                     
                   
                 
                 . 
               
             
           
         
       
     
   
   
     52. The system of  claim 51  wherein during bond formation, the electrons undergo a reentrant oscillatory orbit with vibration of the protons, and the corresponding energy Ē osc  is the difference between the Doppler and average vibrational kinetic energies: 
     
       
         
           
             
               
                 
                   
                     
                       
                         E 
                         _ 
                       
                       osc 
                     
                     = 
                       
                     ⁢ 
                     
                       
                         
                           
                             E 
                             _ 
                           
                           D 
                         
                         + 
                         
                           
                             E 
                             _ 
                           
                           Kvib 
                         
                       
                       = 
                       
                         
                           
                             ( 
                             
                               
                                 V 
                                 e 
                               
                               + 
                               T 
                               + 
                               
                                 V 
                                 m 
                               
                               + 
                               
                                 V 
                                 p 
                               
                             
                             ) 
                           
                           ⁢ 
                           
                             
                               
                                 2 
                                 ⁢ 
                                 
                                   
                                     E 
                                     _ 
                                   
                                   K 
                                 
                               
                               
                                 Mc 
                                 2 
                               
                             
                           
                         
                         + 
                         
                           
                             1 
                             2 
                           
                           ⁢ 
                           ℏ 
                           ⁢ 
                           
                               
                           
                           ⁢ 
                           
                             p 
                             2 
                           
                           ⁢ 
                           
                             
                               k 
                               μ 
                             
                           
                         
                       
                     
                   
                   , 
                   and 
                 
               
             
             
               
                 
                   = 
                     
                   ⁢ 
                   
                     
                       
                         - 
                         
                           p 
                           3 
                         
                       
                       ⁢ 
                       0.326469 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       eV 
                     
                     + 
                     
                       
                         1 
                         2 
                       
                       ⁢ 
                       
                         
                           p 
                           2 
                         
                         ⁡ 
                         
                           ( 
                           
                             0.56764 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             eV 
                           
                           ) 
                         
                       
                     
                   
                 
               
             
           
         
       
     
     The total energy is 
     
       
         
           
             
               
                 
                   
                     E 
                     T 
                   
                   = 
                     
                   ⁢ 
                   
                     
                       V 
                       e 
                     
                     + 
                     T 
                     + 
                     
                       V 
                       m 
                     
                     + 
                     
                       V 
                       P 
                     
                     + 
                     
                       
                         E 
                         _ 
                       
                       osc 
                     
                   
                 
               
             
             
               
                 
                   
                     E 
                     T 
                   
                   = 
                     
                   ⁢ 
                   
                     
                       - 
                       
                         p 
                         2 
                       
                     
                     ⁢ 
                     
                       { 
                       
                         
                           
                             e 
                             2 
                           
                           
                             8 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             π 
                             ⁢ 
                             
                                 
                             
                             ⁢ 
                             
                               ɛ 
                               o 
                             
                             ⁢ 
                             
                               a 
                               O 
                             
                           
                         
                         ⁡ 
                         
                           [ 
                           
                             
                               2 
                               ⁢ 
                               
                                 2 
                               
                             
                             - 
                             
                               2 
                             
                             + 
                             
                               
                                 
                                   2 
                                 
                                 2 
                               
                               ⁢ 
                               ln 
                               ⁢ 
                               
                                 
                                   
                                     2 
                                   
                                   + 
                                   1 
                                 
                                 
                                   
                                     2 
                                   
                                   - 
                                   1 
                                 
                               
                             
                             - 
                             
                               2 
                             
                           
                           ] 
                         
                       
                     
                   
                 
               
             
             
               
                 
                   
                       
                     ⁢ 
                     
                       
                         [ 
                         
                           1 
                           + 
                           
                             p 
                             ⁢ 
                             
                               
                                 
                                   2 
                                   ⁢ 
                                   h 
                                   ⁢ 
                                   
                                     
                                       
                                         e 
                                         2 
                                       
                                       
                                         
                                           
                                             4 
                                             ⁢ 
                                             
                                                 
                                             
                                             ⁢ 
                                             π 
                                             ⁢ 
                                             
                                                 
                                             
                                             ⁢ 
                                             
                                               ɛ 
                                               o 
                                             
                                             ⁢ 
                                             
                                               a 
                                               O 
                                               3 
                                             
                                           
                                           
                                             m 
                                             e 
                                           
                                         
                                         ⁢ 
                                         
                                             
                                         
                                       
                                     
                                   
                                 
                                 
                                   
                                     m 
                                     e 
                                   
                                   ⁢ 
                                   
                                     c 
                                     2 
                                   
                                 
                               
                             
                           
                         
                         ] 
                       
                       - 
                       
                         
                           1 
                           2 
                         
                         ⁢ 
                         h 
                         ⁢ 
                         
                           
                             k 
                             μ 
                           
                         
                       
                     
                     } 
                   
                   . 
                 
               
             
             
               
                 
                   = 
                     
                   ⁢ 
                   
                     
                       
                         - 
                         
                           p 
                           2 
                         
                       
                       ⁢ 
                       31.351 
                       ⁢ 
                       eV 
                     
                     - 
                     
                       
                         p 
                         3 
                       
                       ⁢ 
                       0.326469 
                       ⁢ 
                       eV 
                     
                   
                 
               
             
           
         
       
     
   
   
     53. The system of  claim 52  wherein a bond dissociation energy, E D , is the difference between the total energy of the hydrogen atoms H(1/p) and E T : 
     
       
         
           
             
               
                 
                   
                     E 
                     D 
                   
                   = 
                   
                     
                       E 
                       ⁡ 
                       
                         ( 
                         
                           2 
                           ⁢ 
                           
                             H 
                             ⁡ 
                             
                               ( 
                               
                                 1 
                                 / 
                                 p 
                               
                               ) 
                             
                           
                         
                         ) 
                       
                     
                     - 
                     
                       E 
                       T 
                     
                   
                 
               
             
             
               
                 
                   = 
                   
                     
                       
                         - 
                         
                           p 
                           2 
                         
                       
                       ⁢ 
                       27.20 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       eV 
                     
                     - 
                     
                       E 
                       T 
                     
                   
                 
               
             
             
               
                 
                   = 
                   
                     
                       
                         - 
                         
                           p 
                           2 
                         
                       
                       ⁢ 
                       27.20 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       eV 
                     
                     - 
                     
                       ( 
                       
                         
                           
                             - 
                             
                               p 
                               2 
                             
                           
                           ⁢ 
                           31.351 
                           ⁢ 
                           
                               
                           
                           ⁢ 
                           eV 
                         
                         - 
                         
                           
                             p 
                             3 
                           
                           ⁢ 
                           0.326469 
                           ⁢ 
                           
                               
                           
                           ⁢ 
                           eV 
                         
                       
                       ) 
                     
                   
                 
               
             
             
               
                 
                   = 
                   
                     
                       
                         p 
                         2 
                       
                       ⁢ 
                       4.151 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       eV 
                     
                     + 
                     
                       
                         p 
                         3 
                       
                       ⁢ 
                       0.326469 
                       ⁢ 
                       
                           
                       
                       ⁢ 
                       eV 
                     
                   
                 
               
             
           
         
       
     
     wherein the total energy of two hydrogen atoms H(1/p) is
     E (2 H (1 /p ))=− p   2 27.20 eV.

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